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Q about noise in time interval measurement averging

Discussion in 'Electronic Design' started by colin, Apr 6, 2007.

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  1. colin

    colin Guest

    Hi,
    I have a PIC measuring a time interval to 25ns resolution,
    the interval is totaly asynchronous to the PIC clock.

    So say if I average over 25000 measurements that will give me a limit of 1ps
    resolution.

    Im trying to do a system noise analysis and im wondering how to work this
    out,
    I cant seem to recall how the noise reduces with increasing samples,
    is it 1/samples ? this would be too good to be true,
    or 1/sqrt(samples) this seems rather low.

    there is also a lot of noise in the signal as it is from an optical encoder,
    seems mostly mechanical, I need to reduce this by averaging over a long time
    too.

    Im trying to work out the optimum rate of pulses per revolution to use.

    thanks
    Colin =^.^=
     
  2. Guest

    Noise decreases as one over the square root of the number of samples,
    if the noise on successive samples is uncorrellated.

    The square root of 25000 is 158.1, so you'd reduce your 25nsec
    quantisation error to 158psec rather than 1psec, if you averaged 25000
    independent samples.
    The optimum number of pulses per revolution is probably one, unless
    your need to know the sense of the rotation as well as it's speed.
     
  3. colin

    colin Guest

    Ah yes ofc I must of forgoton how to think for a while,
    I was getting mixed up with the number of available bits for resolution.
    not too woried about the sense of rotation as I know that anyway,
    however im seeing a standard deviation of about 10ns per revolution averaged
    over 2000 pulses per rev,
    Im working on fixing the mechanics to reduce this,
    but 1 pulse per rev would give me 25ns error,

    im looking for .1ps resolution,
    to reduce my SD of 10ns to this amounts to 100000^2 revolutions wich would
    take 3 years at 6000rpm
    id rather it only took a few days, as im not quite that patient.

    3 days would mean i would have to get my SD down to 500ps per rev wich is
    probably highly optimistic
    and id need at least 625 pulses per rev too.

    I could try timing both edges and see how the SD changes with twice as many
    samples.
    I tried feeding the same signal into both A and B, and the SD came out at
    about 25ps
    wich is lower than one would expect but its probably not a valid thing todo.

    the error also seems proportional to 1/shaft speed.

    Colin =^.^=
     
  4. colin

    colin Guest

    ok that making sense now, but I have another question im not sure about,
    that is how to convert that to a noise density,
    I have a slow periodic signal wich im trying to isolate,
    I need to detect its presence and also if possible its magnitude and phase,
    this signal is probably about 0.3ps deviation,
    in the presence of standard deviation of about 10ns.

    So I do a FFT, I need to see the signal significantly above the noise floor,
    the bandwidth is limited by sample rate ~ 100hz to integration time wich is
    many days,
    so say 100hz, is it right to consider the 10ns to be spread out over this
    bandwidth ?

    The FFT I have atm shows lots of spikes,
    so my problem is probably more than just white noise.

    Colin =^.^=
     
  5. joseph2k

    joseph2k Guest

    Your approace should start from statisticel methods. You have the ability
    to get a mean value and the variance (father of standard deviation) from
    that sample size. Compute it out and it should begin to elucidate your
    issues.
     
  6. Fred Bartoli

    Fred Bartoli Guest

    colin a écrit :
    Fun stuff.

    One thing to think about is that when sampling at 100Hz an unlimited BW
    signal you're aliasing all the wideband noise into your 50Hz final BW,
    which won't help S/N ratio.
    You'd have to low pass your time interval signal, either through greater
    sample rate and digital filter it, or maybe you can PLL your signal
    before sampling it.
     
  7. colin

    colin Guest

    "Fred Bartoli"
    hmm im more confused now, the 100hz rate is already an average of 2000 time
    intervals,
    wich is one revolution,

    the period of the signal im looking for is 1 day.
    so the bandwidth is like 0.00001 hz

    Im going to make a program to generate test data so I can mess around and
    see stuff on the FFT.

    The data gets sent to the PC for as serious number crunching as I can dream
    up.

    Colin =^.^=
     
  8. Guest

    The advantage of one pulse per revolution is that you are looking at
    one fiduciary mark on your shaft, so you don't have to worry about the
    spacing of the fiduciary marks around the shaft, or the centering of a
    radially striped disk on the shaft. and the interval between the
    signal edges that define the period of rotation is as long as
    possible, so your quantisation noise is 10nsec in 10msec, rather than
    10nsec in a shorter period.

    If you put an array of detectors around the shaft, so you get one
    pulse per revolution from each sensor, you end up with more
    observations per revolution with independent quantisation noise on
    each value for the period of rotation,

    Obviously, if there is noise on the rate of rotation - such as might
    be caused by a minimally elliptical shaft rotating in a minimally
    elliptical journal bearing - at a frequency that isn't an integral
    multiple of the frequency of rotation, the noise on the output of each
    sensor in the array would be correlated with the noise on the output
    of its nearer neighbours, and averaging wouldn't do as much good as it
    would on uncorrelated noise.

    My own inclination would be to go for a faster clock - using
    Motorola's ECLinPS emitter-coupled logic you could build a very wide
    synchronous counter (you'd need 23 bits - four MC100E016) that could
    follow a 500MHz clock, which would give you 2nsec of jitter rather
    than 25nsec, and drop your three years down to a week.

    Peter Alfke of Xilinx - a guru on comp.arch.fpga - programmed a Xilinx
    programmable logic device to work as a 1GHz counter a few years ago -
    and this might be a better way to go.

    If you were in a position do a serious amount of work, you could
    combine a fast clock with a time-to-voltage converter, and get the
    timing resolution down to around a few tens of picoseconds. Some years
    ago, when I was working on a stroboscopic electron microscope with a
    digital timebase, we set up such a system that digitised time
    intervals with a resolution of 10psec. Our 800MHz clock was not
    crystal-controlled, and our jitter never got better than about 50psec
    before the project was cancelled. I believe that John Larkin (Inland
    Electronics) sells toys that can do better.
     
  9. John  Larkin

    John Larkin Guest

    That's Highland Technology. We're only a streetcar ride from the
    Pacific Ocean.

    But digitizing the output of an encoder to sub-ns resolution is a lost
    cause. Nasty influences, like temperature, bearing wear, led
    degradation, and a host of others will generate a drift floor well
    above that. It would help to know what the op is actually trying to
    do.

    John
     
  10. "so any long term change is ignored" contradicts "the phase
    varies cyclicly over a much longer period wich is the
    measurement of interest."
     
  11. colin

    colin Guest

    well I average all the pulses over exactly one revolution,
    so any eccentricity wich is there should null out in the average.


    I have tried 2 sensors on the same disc, oposite eachother,
    and you can see the error due to disc misalignment etc.
    however averaging this out over 2000 pulses over 1 revolution gave a
    standard deviation of just 500ps.
    wich coresponds well to the reduction of 25ns/sqrt(2000).
    {i had initialy put this down to mechanical/electrical noise}

    Interestingly if I feed it with the same signal as ref and compare it drops
    down to 25ps,
    im not sure if there isnt some peculiarity with the PIC of pulses ariving at
    the same time.
    If I use alternate edges its stil quite low.
    Yes my initial aproach was to use a time to voltage converter,
    but the voltage coresponding to 1ps was very small, and gave rise to its own
    noise problems.

    the other problem wich actually precluded this and make some of the things
    you mentioned much more difficult is that the phase of the 2 signals varies
    by more than 180'.

    I need to keep track of the total phase change, wich might be upto 20
    cycles.
    the PIC handles this surprisingly well, as it timestamps every edge with
    input capture.

    it may stil be possible to do this with a PLD at high clock rate using a
    similar technique.
    however compared to the simple PIC aproach this seems very involved.

    however atm as my mechanical noise is much more than my quantization noise,
    so I think the PIC will suffice.
    I also think the risetime and bandwidth of the electronics and opto devices
    contribute noise wich is best averaged out too, although I have no specs on
    this.

    My main concern at the moment is to re do the mechanical side of things,
    but I needed to know more about how the noise is reduced etc,
    so hopefully I can find room to make it easier to improve the mechanical
    precision
    without losing it in quantisation noise.

    The 10ns noise is mechanical and this is what will cuase it to take 3 years
    to average out.

    with your help I think I understand it well enough now thanks,
    also i did a simulation generating computer data with 10ns variation derived
    by a random number generator,
    the FFT showed a noise floor coresponding to 1/sqrt(samples).

    Although I need to work out how I can reduce this further as my signal has a
    minimal bandwidth.
    im also not exactly a specialist in FFT (yet).

    Colin =^.^=
     
  12. colin

    colin Guest

    Im not so sure, it would just add to the confusion,
    youd probably have lots more questions ...

    basically the signal is cyclic over a few seconds so any long term change is
    ignored,
    the phase varies cyclicly over a much longer period wich is the measurement
    of interest.

    Colin =^.^=
     
  13. colin

    colin Guest

    ha! see i was right, more questions ...
    well the detection of the initial signal is where any long term change in
    the bearings or optics of the encoder should not have any significant
    effect.

    the Phase of this signal should still be preserved if it varies over a
    longer time.

    Colin =^.^=
     
  14. Guest

    That was not a question, but an observation.
     
  15. colin

    colin Guest

    oo good point, It probably wasnt a very good explanation especially given
    that I seemd to have snipped of more than I should of.

    Colin =^.^=
     
  16. Guest

    It is rare for a newby to tell us all we need to know to let us
    produce good answers to their question on the first or second go
    round, but their answers do tend to dimish the confusion, rather than
    adding to it.

    Many of the gurus on this user-group have had a lot of practice at
    going from what the customers think they want to what the customers
    really needs. Some of us have gotten pretty good at it.
    The phase of what relative to what?
     
  17. Ian

    Ian Guest

    Your "two sensors opposite each other" reminded me of a couple of
    techniques: you can use a single source, a light pipe arrangement to
    transfer the optical signal so that it passes through the encoder twice
    at opposite sides of the rotating shaft, and a single receiver.
    This takes out eccentricity effects, and reduces some other things a bit.
    That was a way of commercialising the original idea, which was to do
    a similar thing but distributed all round the rotating shaft. This is a much
    better technique, but more expensive.

    I might still have the original patents kicking around, this was from
    the mid-1970's, I'll have a look tonight.

    Regards
    Ian
     
  18. joseph2k

    joseph2k Guest

    Sounds like loop control systems oscillatory errors. Which may or may not
    be coupled.
     
  19. colin

    colin Guest

    Sorry I dont mean to apear to be shunning your help,
    in fact ive asked questions here about many different parts of this project,
    but its just that if I tell you much more it wont make a lot of sense with
    out telling you a whole lot more,
    wich I dont realy wish to get involved in discussing right now cos im not
    sure I understand the physics behind this or even agree with it !

    I'm not even sure if what im doing is acheivable but then I like a good
    challange every now and then.

    Ive been into electronics since the early 70s,
    although I moved into software as people writing software had an easier job
    and were payed 2-3 times as much.
    not as interesting perhaps.

    however I started by writting device drivers etc,
    and telling disbeleiving hardware engineers how to fix any hardware bugs I
    found was sometimes amusing.
    electronics was delegated to a hobby for some time. Ive ended up being quite
    well skilled in numerous fields, although trying to be expert in so many
    wich this project requires means I end up using the internet a lot.

    Right now ive got to go and get some precision machining done ...
    Think of it like a chopper stabilised op amp, but applied to a mechanical
    system.
    The intermediate cyclic rate is just the chopper frequency,
    this nulls out any offset of phase error and any change of it over a time
    longer than the period.

    The resultant signal, after the chopper part is removed by software, is just
    the value im measuring.
    wich is the response to an input wich is made to vary slowly,
    thereby allowing a complex phase relationship to be measured.

    Colin =^.^=
     
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